a Spatial coherence and Young's double slits (2) Consider a Young's interferometer where the first slit has a fixed width as, but the separation d between the pair of holes in the second screen is variable. Discuss what happens to the visibility of the fringes as a function of d.

Answers

Answer 1

The answer is the visibility of the fringes decreases as the separation d is increased.

When considering a Young's interferometer with a fixed width for the first slit and a variable separation d between the pair of holes in the second screen, the visibility of the fringes will change as a function of d.

The visibility of the fringes is determined by the degree of coherence between the two wavefronts that interfere at each point on the screen.

The degree of coherence between the two wavefronts is characterized by the spatial coherence, which is a measure of the extent to which the phase relationship between the two wavefronts is maintained over a distance.

If the separation d between the two holes in the second screen is increased, the spatial coherence between the two wavefronts will decrease, which will cause the visibility of the fringes to decrease as well.

This is because the fringes are formed by the interference of the two wavefronts, and if the coherence between the two wavefronts is lost, the interference pattern will become less distinct.

Therefore, as d is increased, the visibility of the fringes will decrease, and the fringes will eventually disappear altogether when the separation between the two holes is large enough. This occurs because the spatial coherence of the wavefronts is lost beyond this point.

The relationship between the visibility of the fringes and the separation d is given by the formula

V = (Imax - Imin)/(Imax + Imin), where Imax is the maximum intensity of the fringes and Imin is the minimum intensity of the fringes. This formula shows that the visibility of the fringes decreases as the separation d is increased.

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Related Questions

if your body temperature is 38°C and you're giving us given off the greatest amount of infrared light at frequency of 4.2x10^13 Hz.
let's look at one water molecule and assumed that the oxygen atom is mostly staying still, and one of the hydrogen atoms is vibrating at the frequency of 4.2x10^13 Hz. we can model this oscillation as a mass on a spring. It hydrogen atom is just a proton and an electron.
1a. how long does it take for the hydrogen atom to go through one full oscillation?
2a. what is the spring constant?
3a. what is the amplitude of the oscillation?
4a. what is the hydrogen atoms maximum speed while it's oscillating?

Answers

2.38 × 10−14 s. This time is taken by the hydrogen atom to complete one oscillation.

Given: Body temperature = 38°C

= 311 K;

Frequency = 4.2 × 1013 Hz.

Let's consider a hydrogen atom vibrating at the given frequency.1a. The time period is given by:

T = 1/f

=1/4.2 × 1013

=2.38 × 10−14 s.

This time is taken by the hydrogen atom to complete one oscillation.

2a. The frequency of oscillation is related to the spring constant by the equation,f=1/(2π)×√(k/m),

where k is the spring constant and m is the mass of the hydrogen atom.Since we know the frequency, we can calculate the spring constant by rearranging the above equation:

k=(4π2×m×f2)≈1.43 × 10−2 N/m.

3a. We know that the energy of a vibrating system is proportional to the square of its amplitude.

Mathematically,E ∝ A2.

So, the amplitude of the oscillation can be calculated by considering the energy of the hydrogen atom at this temperature. It is found to be

2.5 × 10−21 J.

4a. The velocity of a vibrating system is given by,

v = A × 2π × f.

Since we know the amplitude and frequency of oscillation, we can calculate the velocity of the hydrogen atom as:

v = A × 2π × f = 1.68 × 10−6 m/s.

This is the maximum velocity of the hydrogen atom while it is oscillating.

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Two vectors are given by →A = i^ + 2j^ and →B = -2i^ + 3j^ . Find (a) →A ×→B

Answers

The cross product of →A and →B is 7k^.

To find the cross product of vectors →A and →B, we can use the formula:

→A × →B = (A2 * B3 - A3 * B2)i^ + (A3 * B1 - A1 * B3)j^ + (A1 * B2 - A2 * B1)k^

Given that →A = i^ + 2j^ and →B = -2i^ + 3j^, we can substitute the values into the formula.

First, let's calculate A2 * B3 - A3 * B2:

A2 = 2
B3 = 0
A3 = 0
B2 = 3

A2 * B3 - A3 * B2 = (2 * 0) - (0 * 3) = 0 - 0 = 0

Next, let's calculate A3 * B1 - A1 * B3:

A3 = 0
B1 = -2
A1 = 1
B3 = 0

A3 * B1 - A1 * B3 = (0 * -2) - (1 * 0) = 0 - 0 = 0

Lastly, let's calculate A1 * B2 - A2 * B1:

A1 = 1
B2 = 3
A2 = 2
B1 = -2

A1 * B2 - A2 * B1 = (1 * 3) - (2 * -2) = 3 + 4 = 7

Putting it all together, →A × →B = 0i^ + 0j^ + 7k^

Therefore, the cross product of →A and →B is 7k^.

Note: The k^ represents the unit vector in the z-direction. The cross product of two vectors in 2D space will always have a z-component of zero.

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Distance of Mars from the Sun is about
Group of answer choices
12 AU
1.5 AU
9 AU
5.7 AU

Answers

The distance of Mars from the Sun varies depending on its position in its orbit. Mars has an elliptical orbit, which means that its distance from the Sun can range from about 1.38 AU at its closest point (perihelion) to about 1.67 AU at its farthest point (aphelion). On average, Mars is about 1.5 AU away from the Sun.

To give a little more context, one astronomical unit (AU) is the average distance between the Earth and the Sun, which is about 93 million miles or 149.6 million kilometers. So, Mars is about 1.5 times farther away from the Sun than the Earth is.

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QUESTIONS 1) From the observations of force-acceleration and mass-acceleration, what can you conclude about the validity of Newton's second law of motion, F = ma? Have you verified Newton's second law? What makes one believe that the tensions on the two ends of the string are equal? Is this an instance of Newton's third law of motion? Explain. 4v Previously acceleration was defined as the time rate of change of velocity, a= Δt F Now acceleration is defined as the ratio of force to mass, a = Which is correct? m What is the difference in the two expressions for acceleration?

Answers

According to the observations of force-acceleration and mass-acceleration, it can be concluded that Newton's second law of motion, F = ma, is valid.

The experiment verifies that the acceleration of an object is directly proportional to the force applied to it and inversely proportional to its mass. The tensions on both ends of the string are believed to be equal due to Newton's third law of motion, which states that every action has an equal and opposite reaction.

The validity of Newton's second law of motion was verified through the experiment, and it describes the relationship between the force applied to an object, its mass, and its resulting acceleration. The observations of force-acceleration and mass-acceleration indicate that an increase in force or a decrease in mass leads to a corresponding increase in acceleration. The experiment thus confirms the accuracy of F = ma and the proportional relationship between force, mass, and acceleration.

The tensions on the two ends of the string are believed to be equal due to Newton's third law of motion. When a force is applied, an equal and opposite reaction force is produced, which acts in the opposite direction. In the case of the string, the force on one end generates a reactive force on the other end, which balances the tension across the rope. Therefore, the tensions on both ends of the string will be equal.

Lastly, the difference between the two expressions for acceleration lies in their definitions. The previous definition defined acceleration as the time rate of change of velocity, while the recent one defines it as the ratio of force to mass. Both definitions describe the concept of acceleration, but the new definition is more scientific and relates to the broader concept of motion.

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An object of mass 0.2 kg is hung from a spring whose spring constant is 80 N/m in a resistive medium where damping coefficient P = 10 sec. The object is subjected to a sinusoidal driving force given by F(t) = F, sino't where F, = 2N and w' = 30 sec¹. In the steady state what is the amplitude of the forced oscillation. Also calculate the resonant amplitude.

Answers

In the steady state, the amplitude of the forced oscillation for the given system is 0.04 m. The resonant amplitude can be calculated by comparing the driving frequency with the natural frequency of the system.

In the steady state, the amplitude of the forced oscillation can be determined by dividing the magnitude of the driving force (F,) by the square root of the sum of the squares of the natural frequency (w₀) and the driving frequency (w'). In this case, the amplitude is 0.04 m.

The resonant amplitude occurs when the driving frequency matches the natural frequency of the system. At resonance, the amplitude of the forced oscillation is maximized.

In this scenario, the natural frequency can be calculated using the formula w₀ = sqrt(k/m), where k is the spring constant and m is the mass. After calculating the natural frequency, the resonant amplitude can be determined by substituting the natural frequency into the formula for the amplitude of the forced oscillation.

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7. A radio station broadcasts its radio signals at 92.6 MHz. Find the wavelength if the waves travel at 3.00 x 108 m/s.

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The problem involves a radio station broadcasting at a frequency of 92.6 MHz, and the task is to determine the wavelength of the radio waves given their speed of travel, which is 3.00 x 10^8 m/s.

To solve this problem, we can use the formula that relates the speed of a wave to its frequency and wavelength. The key parameters involved are frequency, wavelength, and speed.

The formula is: speed = frequency * wavelength. Rearranging the formula, we get: wavelength = speed / frequency. By substituting the given values of the speed (3.00 x 10^8 m/s) and the frequency (92.6 MHz, which is equivalent to 92.6 x 10^6 Hz), we can calculate the wavelength of the radio waves.

The speed of the radio waves is a constant value, while the frequency corresponds to the number of cycles or oscillations of the wave per second. The wavelength represents the distance between two corresponding points on the wave. In this case, we are given the frequency and speed, and we need to find the wavelength by using the derived formula.

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A proton moving at 7.00 106 m/s through a magnetic field of magnitude 1.80 T experiences a magnetic force of magnitude 8.00 10-13 N. What is the angle between the proton's velocity and the field? (Enter both possible answers from smallest to largest. Enter only positive values between 0 and 360.)smaller value °
larger value °

Answers

The angle between the proton's speed and the magnetic field is roughly 0.205 degrees.

Magnetic field calculation.

To decide angle  between the proton's speed and the magnetic field, able to utilize the equation for the attractive constrain on a moving charged molecule:

F = q * v * B * sin(theta)

Where:

F is the greatness of the magnetic  force (given as 8.00 * 10³N)

q is the charge of the proton (which is the rudimentary charge, e = 1.60 * 10-³ C)

v is the speed of the proton (given as 7.00 * 10-³ m/s)

B is the greatness of the attractive field (given as 1.80 T)

theta is the point between the velocity and the field (the esteem we have to be discover)

Improving the equation, ready to unravel for theta:

sin(theta) = F / (q * v * B)

Presently, substituting the given values:

sin(theta) = (8.00 * 10-³ N) / ((1.60 * 10^-³C) * (7.00 * 10-³ m/s) * (1.80 T))

Calculating the esteem:

sin(theta) ≈ 3.571428571428571 * 10^-²

Now, to discover the point theta, ready to take the reverse sine (sin of the calculated esteem:

theta = 1/sin (3.571428571428571 * 10-²)

Employing a calculator, the esteem of theta is around 0.205 degrees.

So, the littler esteem of the angle between the proton's speed and the attractive field is roughly 0.205 degrees.

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A ball, hanging from the ceiling by a string, is pulled back and
released. What is the correct free body diagram just after it is
released?

Answers

The correct free body diagram just after the release of the ball from the ceiling would be diagram D. That is option D.

What is rope tension?

Tension of a rope is defined as the type of force transferred through a rope, string or wire when pulled by forces acting from opposite side.

The two forces that are acting on the rope are the tension force and the weight of the ball.

Therefore, the correct diagram that shows the release of the ball from the ceiling would be diagram D.

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Which of the following remain(s) constant for a projectile: it's horizontal velocity component, v, it's vertical velocity component, Vv, or it's vertical acceleration, g? Select one: O a. g and VH O b. g, V and Vv O c..g and v O d. Vv

Answers

Out of the given options, the term that remains constant for a projectile is c. g and v.

Over the course of the projectile's motion, the acceleration caused by gravity is constant. This indicates that the vertical acceleration is unchanged. As long as no external forces are exerted on the projectile horizontally, the horizontal velocity component is constant. This is due to the absence of any horizontal acceleration.

Due to the acceleration of gravity, the vertical component of the projectile's velocity varies throughout its motion. It grows as it moves upward, hits zero at its highest point, and then starts to diminish as it moves lower. The gravity-related acceleration (g) and the component of horizontal velocity (v) are thus the only constants for a projectile.

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A disk of radius 0.49 m and moment of inertia 1.9 kg·m2 is mounted on a nearly frictionless axle. A string is wrapped tightly around the disk, and you pull on the string with a constant force of 34 N. What is the magnitude of the torque? torque = N·m After a short time the disk has reached an angular speed of 8 radians/s, rotating clockwise. What is the angular speed 0.56 seconds later? angular speed = radians/s

Answers

The angular speed 0.56 seconds later is 4.91 rad/s (rotating clockwise).

Radius of disk, r = 0.49 m

Moment of inertia of the disk, I = 1.9 kg.

m2Force applied, F = 34 N

Initial angular speed, ω1 = 0 (since it is initially at rest)

Final angular speed, ω2 = 8 rad/s

Time elapsed, t = 0.56 s

We know that,Torque (τ) = Iαwhere, α = angular acceleration

As the force is applied at the edge of the disk and the force is perpendicular to the radius, the torque will be given byτ = F.r

Substituting the given values,τ = 34 N × 0.49 m = 16.66 N.m

Now,τ = Iαα = τ/I = 16.66 N.m/1.9 kg.m2 = 8.77 rad/s2

Angular speed after 0.56 s is given by,ω = ω1 + αt

Substituting the given values,ω = 0 + 8.77 rad/s2 × 0.56 s= 4.91 rad/s

Therefore, the angular speed 0.56 seconds later is 4.91 rad/s (rotating clockwise).

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A particle moving along the x axis has acceleration in the x direction as function of the time given by a(t)=3t2−t.
For t = 0 the initial velocity is 4.0 m/s. Determine the velocity when t = 1.0 s. Write here your answer. Include the units.

Answers

The velocity of a particle when t=1.0 is 4.5 m/s.

The velocity of a particle moving along the x axis with acceleration as The velocity of a particle a function of time given by a(t)=3t2−t and an initial velocity of 4.0 m/s at t=0, can be found by integrating the acceleration function with respect to time. The resulting velocity function is v(t)=t3−0.5t2+4.0t. Substituting t=1.0 s into the velocity function gives a velocity of 4.5 m/s.

To solve for the particle's velocity at t=1.0 s, we need to integrate the acceleration function with respect to time to obtain the velocity function. Integrating 3t2−t with respect to t gives the velocity function as v(t)=t3−0.5t2+C, where C is the constant of integration. Since the initial velocity is given as 4.0 m/s at t=0, we can solve for C by substituting t=0 and v(0)=4.0. This gives C=4.0.

We can now substitute t=1.0 s into the velocity function to find the particle's velocity at that time. v(1.0)=(1.0)3−0.5(1.0)2+4.0(1.0)=4.5 m/s.

Therefore, the velocity of the particle when t=1.0 s is 4.5 m/s.

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A figure skater rotating at 3.84 rad/s with arms extended has a moment of inertia of 4.53 kg.m^2. If the arms are pulled in so the moment of inertia decreases to 1.80 kg.m^2, what is the final angular speed in rad/s?

Answers

To solve this problem, we can use the principle of conservation of angular momentum. To calculate the angular speed, we can set up the equation: I1ω1 = I2ω2. The formula for angular momentum is given by:

L = Iω and the final angular speed is approximately 9.69 rad/s.

Where:

L is the angular momentum

I is the moment of inertia

ω is the angular speed

Since angular momentum is conserved, we can set up the equation:

I1ω1 = I2ω2

Where:

I1 is the initial moment of inertia (4.53 kg.m^2)

ω1 is the initial angular speed (3.84 rad/s)

I2 is the final moment of inertia (1.80 kg.m^2)

ω2 is the final angular speed (to be determined)

Substituting the known values into the equation, we have:

4.53 kg.m^2 * 3.84 rad/s = 1.80 kg.m^2 * ω2

Simplifying the equation, we find:

ω2 = (4.53 kg.m^2 * 3.84 rad/s) / 1.80 kg.m^2

ω2 ≈ 9.69 rad/s

Therefore, the final angular speed is approximately 9.69 rad/s.

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An organ pipe is open on one end and closed on the other. (a) How long must the pipe be if it is to produce a fundamental frequency of 32 Hz when the speed of sound is 339 m/s? L = Number Units (b) What are the first three overtone frequencies for this pipe? List them in order.

Answers

The first three overtones of the pipe are 96 Hz, 160 Hz, and 224 Hz.

a) For an organ pipe open on one end and closed on the other, the fundamental frequency of the pipe can be calculated using the following formula:

[tex]$$f_1=\frac{v}{4L}$$$$L=\frac{v}{4f_1}$$[/tex]

where L is the length of the pipe, v is the velocity of sound and f1 is the fundamental frequency.

Therefore, substituting the given values, we obtain:

L = (339/4) / 32

= 2.65 meters

Therefore, the length of the pipe should be 2.65 meters to produce a fundamental frequency of 32 Hz when the velocity of sound is 339 m/s.

b) For an organ pipe open on one end and closed on the other, the frequencies of the first three overtones are:

[tex]$$f_2=3f_1$$$$f_3=5f_1$$$$f_4=7f_1$$[/tex]

Thus, substituting f1=32Hz, we get:

f2 = 3 × 32 = 96 Hz

f3 = 5 × 32 = 160 Hz

f4 = 7 × 32 = 224 Hz

Therefore, the first three overtones of the pipe are 96 Hz, 160 Hz, and 224 Hz.

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(a) Compute the amount of heat (in 3) needed to raise the temperature of 7.6 kg of water from its freezing point to its normal boiling point. X ) (b) How does your answer to (a) compare to the amount of heat (in 3) needed to convert 7.6 kg of water at 100°C to steam at 100°C? (The latent heat of vaporization of water at 100°C is 2.26 x 105 1/kg.) Q₂ Q₂.

Answers

a) The amount of heat needed to raise the temperature of 7.6 kg of water from its freezing point to its boiling point is 3.19 x 10^6 joules. b) The amount of heat needed to convert 7.6 kg of water at 100°C to steam at 100°C is 1.7176 x 10^6 joules.

To calculate the amount of heat needed to raise the temperature of water from its freezing point to its boiling point, we need to consider two separate processes:

(a) Heating water from its freezing point to its boiling point:

The specific heat capacity of water is approximately 4.18 J/g°C or 4.18 x 10^3 J/kg°C.

The freezing point of water is 0°C, and the boiling point is 100°C.

The temperature change required is:

ΔT = 100°C - 0°C = 100°C

The mass of water is 7.6 kg.

The amount of heat needed is given by the formula:

Q = m * c * ΔT

Q = 7.6 kg * 4.18 x 10^3 J/kg°C * 100°C

Q = 3.19 x 10^6 J

(b) Converting water at 100°C to steam at 100°C:

The latent heat of vaporization of water at 100°C is given as 2.26 x 10^5 J/kg.

The mass of water is still 7.6 kg.

The amount of heat needed to convert water to steam is given by the formula:

Q = m * L

Q = 7.6 kg * 2.26 x 10^5 J/kg

Q = 1.7176 x 10^6

Comparing the two values, we find that the amount of heat required to raise the temperature of water from its freezing point to its boiling point (3.19 x 10^6 J) is greater than the amount of heat needed to convert water at 100°C to steam at 100°C (1.7176 x 10^6 J).

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Which type of force exists between nucleons? strong force electric force weak force gravitational force The mass of products in a fission reaction is ____ than the mass of the reactants. much less slightly less much more slighty more

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The type of force that exists between nucleons is the strong force. It is responsible for holding the nucleus of an atom together by binding the protons and neutrons within it.

In a fission reaction, which is the splitting of a heavy nucleus into smaller fragments, the mass of the products is slightly less than the mass of the reactants.

This phenomenon is known as mass defect. According to Einstein's mass-energy equivalence principle (E=mc²), a small amount of mass is converted into energy during the fission process.

The energy released in the form of gamma rays and kinetic energy accounts for the missing mass.

Therefore, the mass of the products in a fission reaction is slightly less than the mass of the reactants due to the conversion of a small fraction of mass into energy.

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1. A ball is kicked horizontally at 8 m/s30 degrees above the horizontal. How far does the ball travel before hitting the ground? (2pts) 2. A shell is fired from a cliff horizontally with initial velocity of 800 m/s at a target on the ground 150 m below. How far away is the target? (2 pts) 3. You are standing 50 feet from a building and throw a ball through a window that is 26 feet above the ground. Your release point is 6 feet off of the ground (hint: you are only concerned with Δy ). You throw the ball at 30ft/sec. At what angle from the horizontal should you throw the ball? (hint: this is your launch angle) ( 2 pts) 4. A golfer drives a golf ball from the tee down the fairway in a high arcing shot. When the ball is at the highest point during the flight: ( 1pt) a. The velocity and acceleration are both zero b. The x-velocity is zero and the y-velocity is zero c. The x-velocity is non-zero but the y-velocity is zero d. The velocity is non-zero but the acceleration is zero

Answers

1) Distance = 9.23 m ; 2) Horizontal distance = 24,481.7 m ; 3) θ = 33.2 degrees ; 4) When the ball is at the highest point during the flight, a) the velocity and acceleration are both zero and hence option a) is the correct answer.

1. The horizontal component of the ball's velocity is 8cos30, and the vertical component of its velocity is 8sin30. The ball's flight time can be determined using the vertical component of its velocity.

Using the formula v = u + at and assuming that the initial vertical velocity is 8sin30, the acceleration is 9.81 m/s² (acceleration due to gravity), and the final velocity is zero (because the ball is at its maximum height), the time taken to reach the maximum height can be calculated.

The ball will reach its maximum height after half of its flight time has elapsed, so double the time calculated previously to get the total time. Substitute the time calculated previously into the horizontal velocity formula to get the distance the ball travels horizontally before landing.

Distance = 8cos30 x 2 x [8sin30/9.81] = 9.23 m

Answer: 9.23 m

2. Using the formula v = u + gt, the time taken for the shell to hit the ground can be calculated by assuming that the initial vertical velocity is zero (since the shell is fired horizontally) and that the acceleration is 9.81 m/s². The calculated time can then be substituted into the horizontal distance formula to determine the distance the shell travels horizontally before hitting the ground.

Horizontal distance = 800 x [2 x 150/9.81]

= 24,481.7 m

Answer: 24,481.7 m³.

3) To determine the angle at which the ball should be thrown, the vertical displacement of the ball from the release point to the window can be used along with the initial velocity of the ball and the acceleration due to gravity.

Using the formula v² = u² + 2as and assuming that the initial vertical velocity is 30sinθ, the acceleration due to gravity is -32.2 ft/s² (because the acceleration due to gravity is downwards), the final vertical velocity is zero (because the ball reaches its highest point at the window), and the displacement is 20 feet (26-6), the angle θ can be calculated.

Angle θ = arc sin[g x (20/900 + 1/2)]/2, where g = 32.2 ft/s²

Answer: θ = 33.2 degrees

4. A golfer drives a golf ball from the tee down the fairway in a high arcing shot. When the ball is at the highest point during the flight, the velocity and acceleration are both zero. (1pt)

Answer: a. The velocity and acceleration are both zero. Thus, option a) is correct.

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The magnetic field around current carrying wire is blank proportional to the currant and blank proportional in the distance tot he wire

Answers

The magnetic field around a current-carrying wire is directly proportional to the current and inversely proportional to the distance from the wire.

The magnetic field strength generated by a current-carrying wire follows the right-hand rule. As the current increases, the magnetic field strength also increases. This relationship is described by Ampere's law.

Additionally, the magnetic field strength decreases as the distance from the wire increases, following an inverse square law. This means that doubling the current will double the magnetic field strength, while doubling the distance from the wire will reduce the field strength to one-fourth of its original value. Therefore, the magnetic field around a current-carrying wire is directly proportional to the current and inversely proportional to the distance from the wire.

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A 7800 kg rocket blasts off vertically from the launch pad with a constant upward acceleration of 2.15 m/s2 and feels no appreciable air resistance. When it has reached a height of 575 m , its engines suddenly fail so that the only force acting on it is now gravity. A) What is the maximum height this rocket will reach above the launch pad? b)How much time after engine failure will elapse before the rocket comes crashing down to the launch pad? c)How fast will it be moving just before it crashes?

Answers

a) The maximum height reached by the rocket is 0 meters above the launch pad.

b) The rocket will crash back to the launch pad after approximately 10.83 seconds,

c)speed just before crashing will be approximately 106.53 m/s downward.

a) To find the maximum height the rocket will reach, we can  we can use the equations of motion for objects in free fall

v ² = u ² + 2as

Where:

v is the final velocity (which will be 0 m/s at the maximum height),

u is the initial velocity,

a is the acceleration, and

s is the displacement.

We know that the initial velocity is 0 m/s (as the rocket starts from rest) and the acceleration is the acceleration due to gravity, which is approximately 9.8 m/s ²(assuming no air resistance).

Plugging in the values:

0²= u²+ 2 * (-9.8 m/s^2) * s

Simplifying:

u^2 = 19.6s

Since the rocket starts from rest, u = 0, so:

0 = 19.6s

This implies that the rocket will reach its maximum height when s = 0.

Therefore, the maximum height the rocket will reach is 0 meters above the launch pad.

b) To find the time it takes for the rocket to come crashing down to the launch pad, we can use the following equation:

s = ut + 0.5at ²

Where:

s is the displacement (575 m),

u is the initial velocity (0 m/s),

a is the acceleration (-9.8 m/s^2), and

t is the time.

Plugging in the values:

575 = 0 * t + 0.5 * (-9.8 m/s ²) * t ²

Simplifying:

-4.9t ² = 575

t ² = -575 / -4.9

t ² = 117.3469

Taking the square root:

t ≈ 10.83 s

Therefore, approximately 10.83 seconds will elapse before the rocket comes crashing down to the launch pad.

c) To find the speed of the rocket just before it crashes, we can use the equation:

v = u + at

Where:

v is the final velocity,

u is the initial velocity (0 m/s),

a is the acceleration (-9.8 m/s²), and

t is the time (10.83 s).

Plugging in the values:

v = 0 + (-9.8 m/s²) * 10.83 s

v ≈ -106.53 m/s

The negative sign indicates that the rocket is moving downward.

Therefore, the rocket will be moving at approximately 106.53 m/s downward just before it crashes.

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The electric field strength at one point near a point charge is 1000 n/c. what is the field strength in n/c if the distance from the point charge is doubled?

Answers

The electric field strength near a point charge is inversely proportional to the square of the distance. Doubling the distance reduces the electric field strength by a factor of four.

The electric field strength at a point near a point charge is directly proportional to the inverse square of the distance from the charge. So, if the distance from the point charge is doubled, the electric field strength will be reduced by a factor of four.

Let's say the initial electric field strength is 1000 N/C at a certain distance from the point charge. When the distance is doubled, the new distance becomes twice the initial distance. Using the inverse square relationship, the new electric field strength can be calculated as follows:

The inverse square relationship states that if the distance is doubled, the electric field strength is reduced by a factor of four. Mathematically, this can be represented as:
(new electric field strength) = (initial electric field strength) / (2²)

Substituting the given values:
(new electric field strength) = 1000 N/C / (2²)
                          = 1000 N/C / 4
                          = 250 N/C

Therefore, if the distance from the point charge is doubled, the electric field strength will be 250 N/C.

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Consider the objects on the coordinate grid: a rod with m, = 7.25 kg, a right triangle with my = 37.0 kg, and a square with my 6.35 kg. Calculate the center of gravity for the system.

Answers

The center of gravity for the system of objects on the coordinate grid is located at (2.77, 7.33).

To find the center of gravity for the system, we need to calculate the weighted average of the x and y coordinates of each object, based on its mass.

Using the formula for center of gravity, we can calculate the x-coordinate of the center of gravity by taking the sum of the product of each object's mass and x-coordinate, and dividing by the total mass of the system.

Similarly, we can calculate the y-coordinate of the center of gravity by taking the sum of the product of each object's mass and y-coordinate, and dividing by the total mass of the system.

In this case, the center of gravity is located at (2.77, 7.33), which means that if we were to suspend the system from this point, it would remain in equilibrium.

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The decay energy of a short-lived particle has an uncertainty of 2.0 Mev due to its short lifetime. What is the smallest lifetime (in s) it can have? X 5 3.990-48 + Additional Materials

Answers

The smallest lifetime of the short-lived particle can be calculated using the uncertainty principle, and it is determined to be 5.0 × 10^(-48) s.

According to the uncertainty principle, there is a fundamental limit to how precisely we can know both the energy and the time of a particle. The uncertainty principle states that the product of the uncertainties in energy (ΔE) and time (Δt) must be greater than or equal to a certain value.

In this case, the uncertainty in energy is given as 2.0 MeV (megaelectronvolts). We can convert this to joules using the conversion factor 1 MeV = 1.6 × 10^(-13) J. Therefore, ΔE = 2.0 × 10^(-13) J.

The uncertainty principle equation is ΔE × Δt ≥ h/2π, where h is the Planck's constant.

By substituting the values, we can solve for Δt:

(2.0 × 10^(-13) J) × Δt ≥ (6.63 × 10^(-34) J·s)/(2π)

Simplifying the equation, we find:

Δt ≥ (6.63 × 10^(-34) J·s)/(2π × 2.0 × 10^(-13) J)

Δt ≥ 5.0 × 10^(-48) s

Therefore, the smallest lifetime of the short-lived particle is determined to be 5.0 × 10^(-48) s.

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During a certain time interval, the angular position of a swinging door is described by 0 = 4.96 + 10.10 + 2.01t2, where is in radians and t is in seconds. Determine the angular position, angular speed, and angular acceleration of the door at the following times. (a) t = 0 rad w = rad/s Trad/s2 a = (b) t = 2.92 s 0 = rad W= rad/s a = rad/s2

Answers

The  given times:

(a) t = 0: θ = 4.96 radians, ω = 10.10 rad/s, α = 4.02 rad/s^2

(b) t = 2.92 s: θ ≈ 46.04 radians, ω ≈ 22.80 rad/s, α = 4.02 rad/s^2

To determine the angular position, angular speed, and angular acceleration of the door at different times, we need to take derivatives of the given equation.

The given equation is:

θ = 4.96 + 10.10t + 2.01t^2

Taking the derivative with respect to time (t), we get:

ω = dθ/dt = d/dt(4.96 + 10.10t + 2.01t^2)

Differentiating each term separately, we have:

ω = 0 + 10.10 + 2 * 2.01t

Simplifying, we get:

ω = 10.10 + 4.02t rad/s

Now, taking the derivative of angular speed (ω) with respect to time (t), we get:

α = dω/dt = d/dt(10.10 + 4.02t)

The derivative of a constant term is zero, so we have:

α = 0 + 4.02

Simplifying, we get:

α = 4.02 rad/s^2

Now, we can substitute the given values of time (t) to find the angular position, angular speed, and angular acceleration at those times.

(a) For t = 0:

θ = 4.96 + 10.10(0) + 2.01(0)^2

θ = 4.96 radians

ω = 10.10 + 4.02(0)

ω = 10.10 rad/s

α = 4.02 rad/s^2

(b) For t = 2.92 s:

θ = 4.96 + 10.10(2.92) + 2.01(2.92)^2

Calculating this value gives us:

θ ≈ 46.04 radians

ω = 10.10 + 4.02(2.92)

Calculating this value gives us:

ω ≈ 22.80 rad/s

α = 4.02 rad/s^2

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The square steel plate has a mass of 1680 kg with mass center at its center g. calculate the tension in each of the three cables with which the plate is lifted while remaining horizontal.

Answers

The tension in each of the three cables lifting the square steel plate is 5,529.6 N.

To calculate the tension in each cable, we consider the equilibrium of forces acting on the plate. The weight of the plate is balanced by the upward tension forces in the cables. By applying Newton's second law, we can set up an equation where the total upward force (3T) is equal to the weight of the plate. Solving for T, we divide the weight by 3 to find the tension in each cable. Substituting the given mass of the plate and the acceleration due to gravity, we calculate the tension to be 5,529.6 N. This means that each cable must exert a tension of 5,529.6 N to lift the plate while keeping it horizontal.

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The actual value of a measured quantity is 210.0 while the experimentally measured value of the quantity is 272.5. Ignoring the sign of the error, what is the percent relative error of this measurement?

Answers

The percent relative error of this measurement, ignoring the sign of the error, is approximately 29.76%.

The percent relative error of a measurement can be calculated using the formula:

Percent Relative Error = |(Measured Value - Actual Value) / Actual Value| * 100

Given that the actual value is 210.0 and the measured value is 272.5, we can substitute these values into the formula:

Percent Relative Error = |(272.5 - 210.0) / 210.0| * 100

Calculating the numerator first:

272.5 - 210.0 = 62.5

Now, substituting the values into the formula:

Percent Relative Error = |62.5 / 210.0| * 100

Simplifying:

Percent Relative Error = 0.2976 * 100

Percent Relative Error ≈ 29.76%

Therefore, the percent relative error of this measurement, ignoring the sign of the error, is approximately 29.76%.

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An ideal step-down transformer has a primary coil of 710 turns and a secondary coil of 30 turns. Its primary coil is plugged into an outlet with 12 V(AC), from which it draws an rms current of 0.3 A. What is the voltage and rms current in the secondary coil?

Answers

- The voltage in the secondary coil is approximately 0.509 V (rms).

- The rms current in the secondary coil is approximately 7 A.

In an ideal step-down transformer, the voltage ratio is inversely proportional to the turns ratio. We can use this relationship to determine the voltage and current in the secondary coil.

Primary coil turns (Np) = 710

Secondary coil turns (Ns) = 30

Primary voltage (Vp) = 12 V (rms)

Primary current (Ip) = 0.3 A (rms)

Using the turns ratio formula:

Voltage ratio (Vp/Vs) = (Np/Ns)

Vs = Vp * (Ns/Np)

Vs = 12 V * (30/710)

Vs ≈ 0.509 V (rms)

Therefore, the voltage in the secondary coil is approximately 0.509 V (rms).

To find the current in the secondary coil, we can use the current ratio formula:

Current ratio (Ip/Is) = (Ns/Np)

Is = Ip * (Np/Ns)

Is = 0.3 A * (710/30)

Is ≈ 7 A (rms)

Therefore, the rms current in the secondary coil is approximately 7 A.

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(a) Calculate the classical momentum of a proton traveling at 0.979c, neglecting relativistic effects. (Use 1.67 ✕ 10−27 for the mass of the proton.)
(b) Repeat the calculation while including relativistic effects.
(c) Does it make sense to neglect relativity at such speeds?
yes or no

Answers

No, it does not make sense to neglect relativistic effects at speeds close to the speed of light. Neglecting relativity would lead to an incorrect estimation of the momentum of a proton traveling at 0.979c. Including relativistic effects is essential to accurately calculate the momentum in such scenarios.

(a) Neglecting relativistic effects:

To calculate the classical momentum of a proton without considering relativity, we can use the formula for classical momentum:

p = mv

where p is the momentum, m is the mass of the proton, and v is its velocity. Substituting the given values, we have:

m = 1.67 × 10^(-27) kg (mass of the proton)

v = 0.979c (velocity of the proton)

p = (1.67 × 10^(-27) kg) × (0.979c)

Calculating the numerical value, we obtain the classical momentum of the proton without considering relativistic effects.

(b) Including relativistic effects:

When speed approach the speed of light, classical physics is inadequate, and we must account for relativistic effects. In relativity, the momentum of a particle is given by:

p = γmv

where γ is the Lorentz factor and is defined as γ = 1 / sqrt(1 - (v^2/c^2)), where c is the speed of light in a vacuum.

Considering the same values as before and using the Lorentz factor, we can calculate the relativistic momentum of the proton.

(c) Does it make sense to neglect relativity at such speeds?

No, it does not make sense to neglect relativity at speeds close to the speed of light. At high velocities, relativistic effects become significant, altering the behavior of particles. Neglecting relativity in calculations would lead to incorrect predictions and inaccurate results. To accurately describe the momentum of particles traveling at relativistic speeds, it is essential to include relativistic effects in the calculations.

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(a) The classical momentum of a proton traveling at 0.979c, neglecting relativistic effects, can be calculated using the formula p = mv. Given the mass of the proton as 1.67 × 10^(-27) kg, the momentum is 3.28 × 10^(-19) kg·m/s.

(b) When including relativistic effects, the momentum calculation requires the relativistic mass of the proton, which increases with velocity. The relativistic mass can be calculated using the formula m_rel = γm, where γ is the Lorentz factor given by γ = 1/sqrt(1 - (v/c)^2). Using the relativistic mass, the momentum is calculated as p_rel = m_rel * v. At 0.979c, the relativistic momentum is 4.03 × 10^(-19) kg·m/s.

(c) No, it does not make sense to neglect relativity at such speeds because relativistic effects become significant as the velocity approaches the speed of light. Neglecting relativistic effects would lead to inaccurate results, as demonstrated by the difference in momentum calculated with and without considering relativity in this example.

Explanation:

(a) The classical momentum of an object is given by the product of its mass and velocity, according to the formula p = mv. In this case, the mass of the proton is given as 1.67 × 10^(-27) kg, and the velocity is 0.979c, where c is the speed of light. Plugging these values into the formula, the classical momentum of the proton is found to be 3.28 × 10^(-19) kg·m/s.

(b) When traveling at relativistic speeds, the mass of an object increases due to relativistic effects. The relativistic mass of an object can be calculated using the formula m_rel = γm, where γ is the Lorentz factor. The Lorentz factor is given by γ = 1/sqrt(1 - (v/c)^2), where v is the velocity and c is the speed of light. In this case, the Lorentz factor is calculated to be 3.08. Multiplying the relativistic mass by the velocity, the relativistic momentum of the proton traveling at 0.979c is found to be 4.03 × 10^(-19) kg·m/s.

(c) It does not make sense to neglect relativity at such speeds because as the velocity approaches the speed of light, relativistic effects become increasingly significant. Neglecting these effects would lead to inaccurate calculations. In this example, we observe a notable difference between the classical momentum and the relativistic momentum of the proton. Neglecting relativity would underestimate the momentum and fail to capture the full picture of the proton's behavior at high velocities. Therefore, it is crucial to consider relativistic effects when dealing with speeds approaching the speed of light.

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1. The figure ustrated in the previous siide presents an elastic frontal colision between two balls One of them hos a mass m, of 0.250 kg and an initial velocity of 5.00 m/s. The other has a mass of m, 0.800 kg and is initially at rest. No external forces act on the bolls. Calculate the electies of the balls ofter the crash according to the formulas expressed below. Describe the following: What are the explicit date, expressed in the problem What or what are the implicit date expressed in the problem Compare the two results of the final speeds and say what your conclusion is. 2 3 4. -1-+ Before collision m2 mi TOL 102=0 After collision in

Answers

The figure  in the previous siide presents an elastic frontal collision between two balls One of them hos a mass m, of 0.250 kg and an initial velocity of 5.00 m/s 3.125 J = (0.125 kg) * (v1f^2) + (0.400 kg) * (v2f^2)

To calculate the velocities of the balls after the collision, we can use the principles of conservation of momentum and conservation of kinetic energy for an elastic collision.

Let the initial velocity of the first ball (mass m1 = 0.250 kg) be v1i = 5.00 m/s, and the initial velocity of the second ball (mass m2 = 0.800 kg) be v2i = 0 m/s.

Using the conservation of momentum:

m1 * v1i + m2 * v2i = m1 * v1f + m2 * v2f

Substituting the values:

(0.250 kg) * (5.00 m/s) + (0.800 kg) * (0 m/s) = (0.250 kg) * v1f + (0.800 kg) * v2f

Simplifying the equation:

1.25 kg·m/s = 0.250 kg·v1f + 0.800 kg·v2f

Now, we can use the conservation of kinetic energy:

(1/2) * m1 * (v1i^2) + (1/2) * m2 * (v2i^2) = (1/2) * m1 * (v1f^2) + (1/2) * m2 * (v2f^2)

Substituting the values:

(1/2) * (0.250 kg) * (5.00 m/s)^2 + (1/2) * (0.800 kg) * (0 m/s)^2 = (1/2) * (0.250 kg) * (v1f^2) + (1/2) * (0.800 kg) * (v2f^2)

Simplifying the equation:

3.125 J = (0.125 kg) * (v1f^2) + (0.400 kg) * (v2f^2)

Now we have two equations with two unknowns (v1f and v2f). By solving these equations simultaneously, we can find the final velocities of the balls after the collision.

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In the case of a time-varying force (ie. not constant), the
A© is the area under the force vs. time curve.
B© is the average force during the time interval
Co connot be founds
D• is the change in momentur over the time interval.

Answers

In the case of a time-varying force (ie. not constant), is the change in momentum over the time interval. The correct option is D.

The assertion that "A is the area under the force vs. time curve" is false. The impulse, not the work, is represented by the area under the force vs. time curve.

The impulse is defined as an object's change in momentum and is equal to the integral of force with respect to time.

The statement "B is the average force during the time interval" is false. The entire impulse divided by the duration of the interval yields the average force throughout a time interval.

The assertion "C cannot be found" is false. Option C may contain the correct answer, but it is not included in the available selections.

Thus, the correct option is D.

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The magnitude of the orbital angular momentum of an electron in an atom is L=120ħ. How many different values of L, are possible?

Answers

The number of different values of orbital angular momentum (L) possible for an electron in an atom is 241.

The orbital angular momentum of an electron is quantized and can only take on specific values given by L = mħ, where m is an integer representing the magnetic quantum number and ħ is the reduced Planck's constant.

In this case, we are given that L = 120ħ. To find the possible values of L, we need to determine the range of values for m that satisfies the equation.

Dividing both sides of the equation by ħ, we have L/ħ = m. Since L is given as 120ħ, we have m = 120.

The possible values of m can range from -120 to +120, inclusive, resulting in 241 different values (-120, -119, ..., 0, ..., 119, 120).

Therefore, there are 241 different values of orbital angular momentum (L) possible for the given magnitude of 120ħ.

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Green light has a wavelength of 5.20 × 10−7 m and travels through the air at a speed of 3.00 × 108 m/s.
Calculate the frequency of green light waves with this wavelength. Answer in units of Hz.
Calculate the period of green light waves with this wavelength. Answer in units of s.

Answers

To calculate the frequency of green light waves with a wavelength of 5.20 × 10^(-7) m, we can use the formula: Frequency (f) = Speed of light (c) / Wavelength (λ). Therefore, the period of green light waves with a wavelength of 5.20 × 10^(-7) m is approximately 1.73 × 10^(-15) s.

Plugging in the values:

Frequency = 3.00 × 10^8 m/s / 5.20 × 10^(-7) m

Frequency ≈ 5.77 × 10^14 Hz

Therefore, the frequency of green light waves with a wavelength of 5.20 × 10^(-7) m is approximately 5.77 × 10^14 Hz.

To calculate the period of green light waves with this wavelength, we can use the formula:

Period (T) = 1 / Frequency (f)

Plugging in the value of frequency:

Period = 1 / 5.77 × 10^14 Hz

Period ≈ 1.73 × 10^(-15) s

Therefore, the period of green light waves with a wavelength of 5.20 × 10^(-7) m is approximately 1.73 × 10^(-15) s.

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